Skip to main content

Bell’s Theorem Tells Us Not What Quantum Mechanics Is, but What Quantum Mechanics Is Not

  • Chapter
  • First Online:
Quantum [Un]Speakables II

Part of the book series: The Frontiers Collection ((FRONTCOLL))

Abstract

Non-locality, or quantum-non-locality, are buzzwords in the community of quantum foundation and information scientists, which purportedly describe the implications of Bell’s theorem. When such phrases are treated seriously, that is it is claimed that Bell’s theorem reveals non-locality as an inherent trait of the quantum description of the micro-world, this leads to logical contradictions, which will be discussed here. In fact, Bell’s theorem, understood as violation of Bell inequalities by quantum predictions, is consistent with Bohr’s notion of complementarity. Thus, if it points to anything, then it is rather the significance of the principle of Bohr, but even this is not a clear implication. Non-locality is a necessary consequence of Bell’s theorem only if we reject complementarity by adopting some form of realism, be it additional hidden variables, additional hidden causes, etc., or counterfactual definiteness. The essay contains two largely independent parts. The first one is addressed to any reader interested in the topic. The second, discussing the notion of local causality, is addressed to people working in the field.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Chapter
USD 29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD 79.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD 99.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD 99.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Institutional subscriptions

Notes

  1. 1.

    The phrases in brackets indicate the text of EPR transformed in such a way so that it fits the considered three-particle example. Their Q (position) is now horizontal component of the spin, and P (momentum) is the vertical one.

  2. 2.

    The mathematical formalism of quantum mechanics reflects complementarity of pairs “observables”. If this is the case say for observables A and B, e.g. describing two different components of spin, then they “do not commute”. This is turn means that in the formal quantum description “operators” associated which the two observables we have the following property: \(AB\ne BA\). Of course complementarity can occur in various degrees. We have perfect complementarity when experiments measuring B give completely random results for quantum systems prepared in any state, which was prepared by measuring A and selecting only systems which gave the same result of this measurement. For example, photons which are selected by a polarization analyzer which allows only linearly polarized photons to pass through it, would upon subsequent measurement of circular polarization give fully random results. Either clockwise or anti-clockwise polarized photons would appear, with equal probabilities. like in a coin toss.

  3. 3.

    Such an approach accepts so called “counterfactual” statements or conditionals. Such statements contain an “if” clause which describes a situation which in fact did not occur: e.g., “If EPR knew the results of the GHZ paper, they would not have written their 1935 work”.

  4. 4.

    EPR forgot that if a new notion is to be introduced to a theory, then it must checked whether it is consistent with all predictions of the theory...

  5. 5.

    “Free will” is usually not a challenged assumption, thus we assume it to hold throughout the discussion.

  6. 6.

    Note already here, that \(\lambda \)’s do not appear in quantum mechanics, thus they are hidden variables. Basically this could already end the discussion, as hidden variables are a program of completing quantum mechanics, just like the aim of EPR. As a matter of fact elements of reality are indeed hidden variables.

  7. 7.

    Some authors reserve the phrase Bell’s second theorem to his independent derivation of the impossibility of non-contextual hidden variables.

  8. 8.

    Of course there is a full mathematical equivalence between local causal theories and stochastic local hidden variable theories of Clauser and Horne. I shall argue that additionally there is no conceptual difference.

  9. 9.

    For a version Bell’s theorem for EPR states see [17], or for a more recent development see [18].

References

  1. D.M. Greenberger, M.A. Horne, A. Zeilinger, in Bell’s Theorem, Quantum Theory, and Conceptions of the Universe, ed. by M. Kafatos (Kluwer Academic, Dordrecht, 1989); D.M. Greenberger, M.A. Horne, A. Shimony, A. Zeilinger, Am. J. Phys. 58, 1131 (1990)

    Google Scholar 

  2. N.D. Mermin, Phys. Today 43(6), 9 (1990)

    Article  Google Scholar 

  3. A. Einstein, B. Podolsky, N. Rosen, Phys. Rev. 47, 777 (1935)

    Article  ADS  Google Scholar 

  4. J.S. Bell, Physics 1, 195 (1964)

    Google Scholar 

  5. See e.g., W.M. de Muynck, W. De Baere, Found. Phys. Lett., 3, 325 (1990), W.M. de Muynck, W. De Baere, H. Martens, Found. Phys. 24, 1589–1664 (1994), A. Stairs, unpublished, http://www.terpconnect.umd.edu/~stairs/papers/EPR_Illusion.pdf

  6. See e.g., T. Norsen, Found. Phys. Lett. 19, 633 (2006), T. Norsen, Against Realism, Found. Phys. 37(3), 311–340 (2007), see also R. Tumulka, Found. Phys. 37, 186 (2007) for a similar approach

    Google Scholar 

  7. N. Bohr, in Essays 1958–1962 on Atomic Physics and Human Knowledge (Wiley, New York, 1963), http://www-physics.lbl.gov/~stapp/Complementarity.doc

  8. C.A. Fuchs, N.D. Mermin, R. Schack, Am. J. Phys. 82(8), 749 (2014)

    Google Scholar 

  9. N. Bohr, Phys. Rev. 48, 696 (1935)

    Article  ADS  Google Scholar 

  10. J.-W. Pan, Z.-B. Chen, C.-Y. Lu, H. Weinfurter, A. Zeilinger, M. Zukowski, Rev. Mod. Phys. 84, 777 (2012)

    Article  ADS  Google Scholar 

  11. J.S. Bell, La nouvelle cuisine, in Speakable and Unspeakable in Quantum Mechanics, 2nd ed. (Cambridge University Press, 2004)

    Google Scholar 

  12. N. Gisin, Found. Phys. 42, 80 (2012)

    Article  ADS  MathSciNet  Google Scholar 

  13. J. Clauser, M. Horne, Phys. Rev. D 10, 526 (1974)

    Article  ADS  Google Scholar 

  14. J.S. Bell, The theory of beables, TH-2053-CERN (1975)

    Google Scholar 

  15. M. Zukowski, Stud. Hist. Phil. Mod. Phys. 36B, 566–575 (2005)

    Article  Google Scholar 

  16. M. Zukowski, C. Brukner, J. Phys. A: Math. Theor. 47, 424009 (2014)

    Article  ADS  MathSciNet  Google Scholar 

  17. K. Banaszek, K. Wodkiewicz, Phys. Rev. A 58, 4345 (1998)

    Article  ADS  Google Scholar 

  18. K. Rosolek, M. Stobinska, M. Wiesniak, M. Zukowski, Phys. Rev. Lett. 114, 100402 (2015)

    Google Scholar 

  19. A. Peres, Am. J. Phys. 46, 747 (1978)

    Article  ADS  Google Scholar 

  20. J.F. Clauser, M.A. Horne, A. Shimony, R.A. Holt, Phys. Rev. Lett. 23, 880 (1969)

    Article  ADS  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to Marek Żukowski .

Editor information

Editors and Affiliations

Rights and permissions

Reprints and permissions

Copyright information

© 2017 Springer International Publishing Switzerland

About this chapter

Cite this chapter

Żukowski, M. (2017). Bell’s Theorem Tells Us Not What Quantum Mechanics Is, but What Quantum Mechanics Is Not . In: Bertlmann, R., Zeilinger, A. (eds) Quantum [Un]Speakables II. The Frontiers Collection. Springer, Cham. https://doi.org/10.1007/978-3-319-38987-5_10

Download citation

Publish with us

Policies and ethics